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Band-asymmetry-driven nonreciprocal electronic transport in a helimagnetic semimetal {\alpha}-EuP$_3$
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abstract
Chiral magnetic textures give rise to unconventional magnetotransport phenomena such as the topological Hall effect and nonreciprocal electronic transport. While the correspondence between real-space magnetic topology/symmetry and such transport phenomena has been well established, a microscopic understanding based on the spin-dependent band structure in momentum space remains elusive. Here we demonstrate how a chiral magnetic structure in real space introduces an asymmetry in the electronic band structure and triggers a nonreciprocal electronic transport in a centrosymmetric helimagnet {\alpha}-EuP$_3$. The magnetic structure of {\alpha}-EuP$_3$ is highly tunable by a magnetic field and closely coupled to its semi-metallic electronic band structure, enabling a systematic study across chiral and achiral magnetic phases on the correspondence between nonreciprocal transport and electronic band asymmetry. Our findings reveal how a microscopic change in the magnetic configuration of charge carriers can lead to nonreciprocal electronic transport, paving the way for designing chiral magnets with desirable properties.
Forward citations
Cited by 3 Pith papers
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Nonreciprocal transport in a room-temperature chiral magnet
Co8Zn9Mn3 shows nonreciprocal resistivity from two coexisting mechanisms, spin-chirality scattering near the Curie temperature and conical-spin band asymmetry at low temperature.
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Coexistence of $p$-wave magnetism and superconductivity
p-wave magnets can coexist with conventional s-wave superconductivity, and the superconducting state strongly enhances the transverse spin current these magnets generate.
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The fate of $p$-wave spin polarization in helimagnets with Rashba spin-orbit coupling
Antiferromagnetically coupled helimagnetic chains preserve p-wave spin polarization under Rashba spin-orbit coupling for any helix period, while single chains only do so for even periods.
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